Provided is a sample image observation device including an SEM and a control system configured to control the SEM. An observation region of a sample is divided into a plurality of sections, and restoration processing is performed on an image which is acquired by irradiating each section with a sparse electron beam, based on scanning characteristics in the section. A reduction in quality of a restored image due to a beam irradiation position deviation caused by a scanning response is prevented and restoration with high accuracy and high throughput under a condition for preventing sample damage is possible.

The purpose of the present invention is to increase accuracy of a specific test using an electronic microscope and improve work efficiency. Provided is a system that identifies test recipe information corresponding to an object to be tested on the basis of attribute information about a testing sample, and analyzes and evaluates the object to be tested contained in the testing sample by checking image data and element analysis data that are acquired by a measuring device in accordance with a control program for the test recipe information, against reference image data and reference element analysis data that are used as evaluation references for the object to be tested.

A scanning electron microscopy (SEM) system is disclosed. The SEM system includes an electron source configured to generate an electron beam and a set of electron optics configured to scan the electron beam across the sample and focus electrons scattered by the sample onto one or more imaging planes. The SEM system includes a first detector module positioned at the one or more imaging planes, wherein the first detector module includes a multipixel solid-state sensor configured to convert scattered particles, such as electrons and/or x-rays, from the sample into a set of equivalent signal charges. The multipixel solid-state sensor is connected to two or more Application Specific Integrated Circuits (ASICs) configured to process the set of signal charges from one or more pixels of the sensor.

An electron microscope includes a stage on which a sample is capable of being placed, a beam generator, a detector, a display, and a controller. The beam generator emits a charged particle beam with which the sample is irradiated. The detector detects a secondary electron or an electron generated from the sample by irradiation with the charged particle beam. The display displays an image of the sample based on a signal from the detector. The controller executes a first irradiation process of specifying a position of a hole bottom by scanning the sample with the charged particle beam when capturing an image of the hole bottom of a hole provided in the sample, and executes a second irradiation process of imaging a shape of the hole bottom by irradiating the hole bottom with the charged particle beam via the hole.

A system and method for defect inspection using voltage contrast in a charged particle system are provided. Some embodiments of the system and method include positioning the stage at a first position to enable a first beam of the plurality of beams to scan a first surface area of the wafer at a first time to generate a first image associated with the first surface area; positioning the stage at a second position to enable a second beam of the plurality of beams to scan the first surface area at a second time to generate a second image associated with the first surface area; and comparing the first image with the second image to enable detecting whether a defect is identified in the first surface area of the wafer.

Method and system for generating a diffraction image comprises acquiring multiple frames from a direct-detection detector responsive to irradiating a sample with an electron beam. Multiple diffraction peaks in the multiple frames are identified. A first dose rate of at least one diffraction peak in the identified diffraction peaks is estimated in the counting mode. If the first dose rate is not greater than a threshold dose rate, a diffraction image including the diffraction peak is generated by counting electron detection events. Values of pixels belonging to the diffraction peak are determined with a first set of counting parameter values corresponding to a first coincidence area. Values of pixels not belonging to any of the multiple diffraction peaks are determined using a second, set of counting parameter values corresponding to a second, different, coincidence area.

Systems and methods for automated sample alignment for microscopy are described herein. In one aspect a method can include: rotating the sample along a first axis by each of a plurality of rotation angles; imaging, with a charged particle beam, the sample for each rotation angle; and determining a first rotation angle based on the image for each rotation angle, wherein the first rotation angle aligns the sample to the charged particle beam in relation to the first axis; and determining a second rotation angle based on the first rotation angle, where the second rotation angle aligns the sample to the charged particle beam in relation to a second axis, and where the second axis is orthogonal to the first axis

Analyzing a buried layer on a sample includes milling a spot on the sample using a charged particle beam of a focused ion beam (FIB) column to expose the buried layer along a sidewall of the spot. From a first perspective a first distance is measured between a first point on the sidewall corresponding to an upper surface of the buried layer and a second point on the sidewall corresponding to a lower surface of the buried layer. From a second perspective a second distance is measured between the first point on the sidewall corresponding to the upper surface of the buried layer and the second point on the sidewall corresponding to the lower surface of the buried layer. A thickness of the buried layer is determined using the first distance and the second distance.

An observation apparatus and method that avoids drawbacks of a Lorentz method and observes a weak scatterer or a phase object with in-focus, high resolution, and no azimuth dependency, by a Foucault method observation using a hollow-cone illumination that orbits and illuminates an incident electron beam having a predetermined inclination angle, an electron wave is converged at a position (height) of an aperture plate downstream of a sample, and a bright field condition in which a direct transmitted electron wave of the sample passes through the aperture plate, a dark field condition in which the transmitted electron wave is shielded, and a Schlieren condition in which approximately half of the transmitted wave is shielded as a boundary condition of both of the above conditions are controlled, and a spatial resolution of the observation image is controlled by selecting multiple diameters and shapes of the opening of the aperture plate.

Provided is a charged particle beam device capable of improving the accuracy of measurement and processing. The charged particle beam device includes an electrostatic chuck that adsorbs an inspection object, a voltage generation unit that generates a voltage to be supplied to the electrostatic chuck, and a state determination unit that determines a state of the inspection object. Here, the state determination unit includes a current waveform simulation unit that simulates a time-series change of an electrostatic chuck current flowing through the voltage generation unit when the electrostatic chuck normally adsorbs the inspection object, a difference integration unit that acquires an integration value of a difference between a time-series change of a simulation current generated by the current waveform simulation unit and the time-series change of the electrostatic chuck current flowing through the voltage generation unit, and a difference determination unit that determines an adsorption state of the inspection object and a shape feature of the inspection object based on the integration value of the difference.